Discovery of 10,059 three-dimensional periodic orbits for the general three-body problem

Xiaoming LI and Shijun LIAO

A very few three-dimensional (3D) periodic orbits of general three-body problem (with three finite masses) have been discovered since Newton mentioned it in 1680s. Using a high-accuracy numerical strategy we discovered 10,059 three-dimensional periodic orbits of the three-body problem in the cases of m1=m2=1 and m3=0.1*n where 1≤n≤20 is an integer, among which 1,996 (about 20%) are linearly stable. Note that our approach is valid for arbitrary mass m3 so that in theory we can gain an arbitrarily large amount of 3D periodic orbits of the three-body problem. In the case of three equal masses, we discovered twenty-one 3D “choerographical” periodic orbits whose three bodies move periodically in a single closed orbit. It is very interesting that, in the case of two equal masses, we discovered 273 three-dimensional periodic orbits with the two bodies (m1=m2=1) moving along a single closed orbit and the third (m3 is not equal to 1) along a different one: we name them “piano-trio” orbits, like a trio for two violins and one piano. To the best of our knowledge, all of these 3D periodic orbits have never been reported, indicating the novelty of this work. The large amount of these new 3D periodic orbits are helpful for us to have better understandings about chaotic properties of the famous three-body problem, which “are, so to say, the only opening through which we can try to penetrate in a place which, up to now, was supposed to be inaccessible”, as pointed out by Poincare, the founder of chaos theory.

For detailed initial conditions and topological sequences, please refer to the following supplementary datasets:

(A) Initial conditions of periodic orbits in the 3D three-body problem; Initial conditions of piano-trio orbits in the 3D three-body problem.

(B) Topological sequences of periodic orbits in the 3D three-body problem.

fig2a fig2b fig2c fig2d fig2e fig2f
FIG1. 3D periodic orbits of general three-body problem: (a) $O_{2}(1.2)$, (b) $O_{8}(0.6)$, (c) $O_{3}(1.0)$, (d) $O_{4}(1.0)$, (e) $O_{6}(1.0)$, (f) $O_{6}(1.2)$. Blue circle: Body-1; Red circle: Body-2; Green circle: Body-3.
fig3a fig3b fig3c fig3d
FIG2. 3D choreographic periodic orbits of three-body problem in the case of m1=m2=m3=1: (a) $O_{62}(1.0)$, (b) $O_{64}(1.0)$, (c) $O_{231}(1.0)$, (d) $O_{524}(1.0)$. Three bodies move along a single closed orbit (green). Blue circle: Body-1; Red circle: Body-2; Green circle: Body-3.
fig4a fig4b fig4c fig4d
FIG3. 3D “piano-trio orbits” of three-body problem with two bodies (m1=m2=1) moving along a single closed orbit (red) but the third (m3 ≠ 1) along a distinct orbit (green): (a) $O_{6}(0.6)$, (b) $O_{26}(1.1)$, (c) $O_{48}(0.5)$, (d) $O_{267}(0.9)$. Blue circle: Body-1 (m1=1); Red circle: Body-2 (m2=1); Green circle: Body-3 (m3 ≠ 1).
✦ Visualization for all three-dimensional periodic three-body orbits ✦
Physical Space
Shape Sphere
Mass m₃
Orbit
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